BACKGROUND OF THE INVENTION
1. Field of the Invention
[0001] The present invention relates generally to optical systems, and more particularly,
to a high efficiency polarization device for converting substantially all incoming
light into a single polarization.
2. Description of the Related Art
[0002] Applications that use liquid crystal cells to render an image usually require linearly
polarized input light to function properly. Conventional light sources are typically
unpolarized. In order to polarize this light, it is passed through a polarizer, which
transmits the desired polarization state and absorbs or deflects the unusable, perpendicular
polarization state. Thus, approximately half of the incoming source light has to be
discarded, resulting in reduced system efficiency and brightness.
[0003] Solutions to the foregoing efficiency problem have been developed to transform the
light from the unusable polarization state into the desired state. One solution developed
by 3M Company is a dual brightness enhancement film which is used in laptop LCD displays
to increase screen brightness. The film transmits the desired polarization state and
reflects the perpendicular polarization state back to the light source. Due to scatter
and reflection, part of this light is reflected back in the desired polarization state
and passes to the screen. However, due to high brightness requirements and light absorption
in the source, this approach is of limited efficiency for use in LCD projection applications.
[0004] Another solution in the art is the use of a polarizing beam splitter of the type
shown in Fig. 1. Unpolarized light 10 is directed to a polarizing beam splitter 12.
A desired light polarization is transmitted by the polarizing beam splitter 12 and
is represented by the light beam 14. The polarizing beam splitter 12 reflects the
perpendicular state of polarization. This reflected perpendicular state of polarization
is then directed by a mirror 16 through a half wave plate 18, which functions to change
the polarization state of the reflected light into light 20 with the desired state
of polarization. In theory, the total amount of unpolarized incoming light is transformed
into linearly polarized light. However, the resulting light consists of two distinct
optical beams, which are difficult to utilize in an optical system. Large and more
expensive optics would be required in order to facilitate the utilization of both
beams, and the optical efficiency of such a complex system would typically not be
optimum. Accordingly, there continues to be an efficiency problem in the conversion
of light to a single polarization.
SUMMARY OF THE INVENTION
[0005] Briefly, the present invention comprises, in one embodiment, a polarization device
comprising: a light path; a micro lens array disposed in the light path for separating
light into a plurality of individual beams of light; a polarization filter disposed
in the light path to receive a plurality of the beams of light and to transmit the
received light of a desired polarization state and reflect the received light of a
perpendicular polarization state that is perpendicular to the desired polarization
state; and a reflecting polarization converter disposed to receive and reflect the
reflected light of the perpendicular polarization state and to convert the perpendicular
polarization state to the desired polarization state.
[0006] In a further aspect of the present invention, the polarization filter is shaped to
reflect the light of the perpendicular polarization state in each of a plurality of
the individual beams of light from the micro lens array so that they do not substantially
propagate back exactly in the direction from which they have come.
[0007] In a further aspect of the present invention, the reflecting polarization converter
is disposed in the light path between the micro lens array and the polarization filter
and includes a plurality of transmissive regions, each of a plurality of the transmissive
regions being aligned with a different one of the plurality of beams of light from
the micro lens array to transmit the beam of light aligned therewith.
[0008] In a further aspect of the present invention, the polarization filter is shaped to
reflect the light of the perpendicular polarization state of each of a plurality of
the individual beams of light from the micro lens array at an angle so that the beam
is not substantially reflected straight back through the transmissive region aligned
therewith and so that each of the reflected individual beams of light impinges on
an area on the reflecting polarization converter adjacent to the transmissive region.
[0009] In yet a further aspect of the present invention, the transmissive regions are formed
by holes in the reflecting polarization converter.
[0010] In a further aspect of the present invention, the reflecting polarization converter
comprises a quarter wave plate with a reflective surface disposed thereon with the
transmissive regions comprising openings defined in the reflective surface.
[0011] In a further aspect of the present invention, the polarization filter has a plurality
of features therein, each shaped to reflect light from a different one of the individual
beams of light to a different particular area on the reflecting polarization converter.
[0012] In a yet further aspect of the present invention, each of the features on the polarization
filter has a centerline, each of the micro lenses in the micro lens array has a centerline,
and each of the transmissive regions in the reflecting polarization converter has
a centerline, and wherein each a plurality of the micro lenses has its centerline
aligned with the centerline for one of the transmissive regions and with the centerline
for one of the features of the polarization filter.
[0013] In a further aspect of the present invention, the reflecting polarization converter
includes a reflective surface disposed on one face of a quarter wave plate.
[0014] In a further aspect of the present invention, a shape and angle of the polarization
filter and a shape and angle of the reflecting polarization converter cause light
reflected from the reflecting polarization filter to have substantially a same range
of emission angles as the light of the desired polarization state transmitted by the
polarization filter.
[0015] In a further embodiment of the present invention, a method is provided for polarizing
light comprising the steps of: separating light in a light path into a plurality of
individual beams of light; filtering the plurality of individual beams of light into
light beams with a desired polarization state and light beams with a polarization
state substantially perpendicular to the desired polarization state; transmitting,
with a first range of emission angles, the light beams of the desired polarization
state, and reflecting the light beams with the substantially perpendicular polarization
state; and re-reflecting the reflected light beams of the substantially perpendicular
polarization state and converting the perpendicular polarization state thereof to
the desired polarization state, the re-reflected light beam having substantially a
same range of emission angles as the first range of emission angles of the transmitted
light beam of the desired polarization state.
[0016] In a further aspect of the present invention, the method further comprises the step
of passing each of a plurality of the individual beams of light through a different
associated transmissive region in an element operating to perform the re-reflecting
and converting step, prior to the filtering step; and wherein the reflecting step
comprises the step of reflecting each of the light beams of the substantially perpendicular
polarization state, not straight back into the transmissive region associated with
the light beam, but onto a surface surrounding the associated transmissive region
in the element, and wherein the re-reflecting step occurs on the surface.
BRIEF DESCRIPTION OF THE DRAWINGS
[0017] Fig. 1 is a schematic block diagram of an embodiment of the prior art.
[0018] Fig. 2 is a schematic block diagram of a first embodiment of the present invention.
[0019] Fig. 3 is a schematic block diagram of a preferred embodiment of the present invention.
[0020] Fig. 4 is a schematic diagram of a reflector or mirror surface that may be used in
forming the polarization filter.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
[0021] Referring now to Fig. 2, there is shown a first embodiment of the present invention.
Incoming unpolarized light 30 is directed to a micro lens array 32 that operates to
separate the incoming unpolarized light 30 into a multitude of individual beams 34.
A variety of different types of micro lens array 32 are available for implementing
the present invention, and example parameters for such arrays will be discussed below.
As described by fundamental optics, the divergence of each of the individual beams
created by the individual lenses in the micro lens array 32 will be larger than the
divergence of the original beam 30.
[0022] A polarization filter 38 is disposed in the light path of the light beams 34. The
polarization filter 38 transmits with a given range of emission angles received light
37 of a desired polarization state, while substantially reflecting that received light
39 that has a polarization state that is perpendicular to the desired polarization
state. By way of example, this polarization filter 38 may be comprised of a formable
film for separating the perpendicular polarizations. Dual brightness enhancement film
made by 3M Company, or alternatively any device which performs polarization separation
filtering may be utilized to implement the polarization filter 38.
[0023] In a preferred embodiment, the polarization filter 38 is formed to include a plurality
of features 44 shaped so as not to reflect the perpendicular polarization of an individual
beam straight back in the direction from which it has come, but rather to a designated
region on a reflecting polarization converter 40.
[0024] In a preferred embodiment, the individual beams 34 propagate through the reflecting
polarization converter 40 in order to reach the polarization filter 38. To accomplish
this propagation, the reflecting polarization element 40 includes an array of transmissive
regions 36, with each transmissive region aligned with a different beam 34. The size
of each of the transmissive regions 36 in the reflecting polarization converter 40
approximates the waist of the individual beams 34 in order to ensure maximum transmission
of the individual beams 34 by the transmissive regions 36. Accordingly, the transmissive
regions 36 in the reflecting polarization converter 40 are preferably on the same
scale as the micro lenses in the micro lens array 32, with the transmissive region
centerline to centerline spacing being substantially the same as the centerline to
centerline spacing between micro lenses in the micro lens array 32. The transmissive
regions 36 may be formed simply by making holes extending through the reflecting polarization
converter 40 of the appropriate diameter aligned with the individual micro lenses.
This implementation of the transmissive regions 36 is shown in Fig. 2. Alternatively,
in a preferred embodiment, the transmissive regions 36 may be formed in the reflecting
polarization converter 40 by forming regions of the appropriate size with no reflective
backing aligned with individual micro lenses for transmitting the individual beams
to the polarization filter 38. This embodiment of the transmissive regions 36 is shown
in Fig. 3.
[0025] As noted above, in the preferred embodiment, the polarization filter 38 functions
to reflect light of the perpendicular polarization so that it does not propagate straight
back through the transmissive region 36 from which the light beam has come, but rather
to a particular area on the reflecting polarization converter 40. In a preferred embodiment,
the features 44 shown in Fig. 2 are two-sided sawtooths or four-sided pyramids to
reflect the perpendicular polarization of the light beam to a surface of the reflecting
polarization converter 40 to the sides adjacent to the transmissive region 36 through
which that beam 34 had initially propagated. It can be seen that there are a plurality
of sawtooths or pyramids shown in Fig. 2, each sawtooth or pyramid with its apex centerline
aligned with the centerline of a different transmissive region 36 and the centerline
of a different micro lens in the micro lens array 32. The feature 44 is constructed
on the scale of the micro lens, with the centerline to centerline distance being substantially
the same as the centerline to centerline spacing of the micro lens array 32. Fig.
4 shows a top view of the features 44 on the polarization filter 38 configured as
a matrix of four-sided pyramids. Note that although the feature 44 is illustrated
in the top view in Fig. 4 as a pyramid, the present invention could be implemented
with any feature shape that appropriately reflects the perpendicular polarization
to a desired surface on the reflecting polarization converter 40 including cone shapes,
hemispherical-type shapes, aspherical shapes and asymmetric shapes. Note that cone,
hemispherical, aspherical and asymmetrical features would require more complex shapes
for the surface. Also, note the scale of Fig. 4 is not identical in scale to Fig.
3 for ease of illustration.
[0026] The reflecting polarization converter 40 is disposed to re-reflect the reflected
light of the perpendicular polarization state and to convert that perpendicular polarization
state to the desired polarization state. In a preferred embodiment, the reflecting
polarization converter 40 is implemented simply by using a quarter wave plate element
43 with a mirror backing 46 as the base structure, with the transmissive regions 36
formed by not having a mirror backing in those regions. The preferred embodiment with
the transmissive regions 36 formed in this manner is shown in Fig. 3. The mirror backing
46 for the reflecting polarization converter 40 may be deposited on a quarter wave
plate with appropriate masking techniques used to define the transmissive regions
36 and keep them clear of the mirror material. Alternatively, the mirror or other
reflecting material 46 may be formed as a sheet with openings therein defining the
transmissive regions 36. This mirror sheet 46 may then be affixed or disposed adjacent
to and parallel to the quarter wave plate to form the reflecting polarization converter
40 with the transmissive regions 36 formed therein. Fig. 3 illustrates a mirror surface
46, formed either as a deposition on a surface of a quarter wave plate or a separate
sheet affixed or supported parallel to one surface of the quarter wave plate 43, with
transmissive regions 36 formed therein that contain no reflective material.
[0027] In operation, light beam 39 reflected back by the polarization filter 38 impinges
upon the quarter wave plate 43 in the reflecting polarization converter 40, propagates
through the quarter wave plate 43 to the reflective mirror backing 46 deposited, affixed,
or supported adjacent to the quarter wave plate 43, and is reflected back through
the quarter wave plate 43 by the mirror backing. Accordingly, light beam 39 reflected
by the polarization filter 38 passes twice through the quarter wave plate 43, thereby
converting a perpendicular polarization state to light rays 42 having the desired
polarization state. Note that the polarization filter 38 will not be an impediment
to the re-reflected light rays 42 because the reflected light rays have now been converted
to a polarization state that will be passed through the filter 38. Subsequent optics
(not shown) are then provided to gather the light beams 37 and 42 and refocus them
in a well-known manner.
[0028] It should be noted that the range of emission angles of the beam 42 reflected by
the mirror surface 46 of the reflecting polarization converter 40 depends on the geometries,
for example the shape and angle, of the features 44 of the polarization filter 38,
and on the geometries of the areas around the transmissive regions 36 in the reflecting
polarization converter 40. Note that each instance of an area around a transmissive
region 36 in the reflecting polarization converter 40 may take a spherical shape,
an aspherical shape, or an asymmetric shape. Accordingly, the geometries of the polarization
filter 38 and the reflecting polarization converter 40 can be optimized to cause the
resulting converted light beams 42 to have a range of emission angles very close to
the range of emission angles of the original transmitted light 37 with the desired
polarization, i.e., they have a substantially similar angular distribution of rays.
This optimization can be accomplished by shaping the elements 38 and/or 40 and empirically
determining the optimum shapes. Alternatively, software design programs such as ZEMAX
or ASAP may be utilized in this optimization process. Thus, this system can convert
a beam of unpolarized light with high efficiency into a beam of polarized light with
a size close to the size of the original beam. It should be noted that the drawn shapes
of the elements 38 and 40 are for ease of illustration only and are not to scale.
It should also be noted that the angles shown for the light beams 37 and 42 are for
ease of illustration only.
[0029] In a preferred embodiment of the present invention, each micro lens in the micro
lens array 32 may be implemented to have a focal length of on the order of 1 mm with
a diameter of the micro lens of on the order of 100 microns, and with a spacing between
lenses of on the order of 100 microns. It should be noted that the micro lens parameters
comprising the focal length, the diameter of the lenses, and the number of lenses
per unit length may be optimized empirically to achieve a maximum light polarization
efficiency. As a general rule, the spacing of the centers of the individual micro
lenses in the micro lens array 32 will be substantially identical to and coincide
with the spacing and location of the centers of the transmissive regions 36 in the
reflecting polarization converter 40, with a different transmissive region 36 being
provided for each of a plurality of the micro lenses in the micro lens array 32. Note
that the diameter of each of the transmissive regions 36 in the reflecting polarization
converter 40 preferably will be the diameter of the focused beam 34, and thus will
depend on the optical characteristics of the lenses used in the micro lens array 32.
By way of example, micro lens arrays designed by 3M or by NEC Optics may be utilized
to implement the present invention.
[0030] As noted above, in order to optimize the polarization device of the present invention,
the polarization filter 38 or its functional equivalent and/or the reflecting polarization
converter 40 should be shaped so as to guide the reflected light beams 42 along paths
that are substantially parallel to the unreflected light beams 37, i.e., having a
substantially similar angular distribution of rays, but offset from the light beam
37 by ½ the lens array spacing. The number of lenses in the micro lens array 32 must
be large enough so that the resulting beam comprising the unreflected light bundles
37 and the reflected/converted light bundles 42 fills with sufficient uniformity the
etendue of the optical transport system that follows the device. This optimization
will depend on the characteristics of the subsequent optical transport system, and
therefore cannot be specified in advance.
[0031] The present invention provides a method of transforming unpolarized light into polarized
light with high efficiency. The polarized light resulting from the present invention
is contained in a single beam with a size close to the original unpolarized beam.
This contrasts with the prior art where the original beam is expanded to twice its
original size in order to obtain all of the light in a single polarization. Thus,
the present invention provides light which can be easily utilized in optical systems
resulting in higher system efficiency and less complexity than would otherwise be
required to improve beam properties.
[0032] The foregoing description of a preferred embodiment of the invention has been presented
for purposes of illustration and description. It is not intended to be exhaustive
or to limit the invention to the precise form disclosed, and modifications and variations
are possible in light of the above teachings or may be acquired from practice of the
invention. The embodiment was chosen and described in order to explain the principles
of the invention and its practical application to enable one skilled in the art to
utilize the invention in various embodiments and with various modifications as are
suited to the particular use contemplated. It is intended that the scope of the invention
be defined by the claims appended hereto, and their equivalents.
1. A polarization device comprising:
a light path;
a micro lens array (32) disposed in said light path for separating light into a plurality
of individual beams of light;
a polarization filter (38) disposed in said light path to receive a plurality of said
beams of light and to transmit said received light of a desired polarization state
and reflect said received light of a perpendicular polarization state that is perpendicular
to said desired polarization state; and
a reflecting polarization converter (40) disposed to receive and reflect said reflected
light of said perpendicular polarization state and to convert said perpendicular polarization
state to said desired polarization state.
2. A device as defined in claim 1, wherein said polarization filter (38) is shaped to
reflect said light of said perpendicular polarization state in each of a plurality
of said individual beams of light from said micro lens array so that they do not substantially
propagate back exactly in the direction from which they have come.
3. A device as defined in claim 1 or 2, wherein said reflecting polarization converter
is disposed in said light path between said micro lens array and said polarization
filter and includes a plurality of transmissive regions (36), each of a plurality
of said transmissive regions being aligned with a different one of said plurality
of beams of light from said micro lens array to transmit said beam of light aligned
therewith.
4. A device as defined in claim 3, wherein said polarization filter is shaped (44) to
reflect said light of said perpendicular polarization state of each of a plurality
of said individual beams of light from said micro lens array at an angle so that it
is not substantially reflected straight back through said transmissive region aligned
therewith and so that each of said reflected individual'beams of light impinges on
an area on said reflecting polarization converter adjacent said transmissive region.
5. A device as defined in claim 3 or claim 4, wherein said transmissive regions (36)
are formed by holes in said reflecting polarization converter.
6. A device as defined in one of claims 3 to 5, wherein said reflecting polarization
converter comprises a quarter wave plate (43) and a reflective surface (46) disposed
parallel thereto with said transmissive regions (36) comprising openings defined in
said reflective surface.
7. A device as defined in claim 6, wherein said reflective surface is disposed on said
quarter wave plate.
8. A device as defined in one of claims 3 to 7, wherein said polarization filter has
a plurality of features (44) therein, each shaped to reflect light from a different
one of said individual beams of light to a particular area on said reflecting polarization
converter adjacent to said transmissive region.
9. A device as defined in claim 8, wherein each of said features (44) on said polarization
filter has a centerline, each of said micro lenses in said micro lens array has a
centerline, and each of said transmissive regions (36) in said reflecting polarization
converter has a centerline, and wherein each of a plurality of said micro lenses has
its centerline aligned with the centerline for one of said transmissive regions and
with the centerline for one of said features of said polarization filter.
10. A device as defined in claim 9, wherein said feature (44) comprises a sawtooth shape
disposed to project toward said transmissive region aligned therewith.
11. A device as defined in claim 9, wherein said feature (44) comprises a pyramid shape
disposed to project toward said transmissive region aligned therewith.
12. A device as defined in claim 1 or claim 2, wherein said reflecting polarization converter
includes a reflective surface (46) disposed on one face of a quarter wave plate (43).
13. A device as defined in one of the preceding claims, wherein a geometry of said polarization
filter and a geometry of said reflecting polarization converter cause light reflected
from said reflecting polarization filter to have substantially a same range of emission
angles as said light of said desired polarization state transmitted by said polarization
filter.
14. A method for polarizing light comprising the steps of:
separating light in a light path into a plurality of individual beams of light;
filtering said plurality of individual beams of light into light beams with a desired
polarization state and light beams with a polarization state substantially perpendicular
to said desired polarization state;
transmitting, with a first range of emission angles, said light beams of said desired
polarization state, and reflecting said light beams with said substantially perpendicular
polarization state; and
re-reflecting said reflected light beams of said substantially perpendicular polarization
state and converting said perpendicular polarization state thereof to said desired
polarization state, said re-reflected light beam having substantially a same range
of emission angles as said first range of emission angles of said transmitted light
beam of said desired polarization state.
15. A method as defined in claim 14, further comprising the step of passing each of a
plurality of said individual beams of light through a different associated transmissive
region (36) in an element (40) operating to perform the re-reflecting and converting
step, prior to said filtering step; and wherein said reflecting step comprises the
step of reflecting each of said light beams of said substantially perpendicular polarization
state, not straight back into said transmissive region associated with said light
beam, but onto a surface adjacent said associated transmissive region in said element,
and wherein said re-reflecting step occurs on said surface.